TOPICS
Search

Two-Body Problem


The two-body problem is the n-body problem for two bodies of masses m_1,m_2>0 under mutual Newtonian gravitational attraction. Their center of mass moves with constant velocity, while their relative position vector r=r_1-r_2 satisfies

 r^..=-(G(m_1+m_2))/(||r||^3)r,

where G is the gravitational constant (Heggie 2006).

If the specific angular momentum h=r×r^. is nonzero, the motion lies in a plane perpendicular to h. In polar coordinates, with the angular origin chosen along the direction of closest approach,

 r(theta)=p/(1+ecostheta),

where p=||h||^2/[G(m_1+m_2)] and e>=0 is the eccentricity. The trajectory is an ellipse for e<1, a parabola for e=1, and a hyperbola for e>1. The case e=0 is a circle; zero angular momentum instead gives radial motion.

By Newton's shell theorem, the same exterior interaction applies to two bodies with spherically symmetric mass distributions whose centers are separated by more than the sum of their outer radii.


See also

Center of Mass, Conic Section, Eccentricity, n-Body Problem, Newton's Shell Theorem, Three-Body Problem

Explore with Wolfram|Alpha

References

Heggie, D. C. "Gravitational N-Body Problem (Classical)." In Encyclopedia of Mathematical Physics (Ed. J.-P. Françoise, G. L. Naber, and S. T. Tsou). Oxford, England: Elsevier, pp. 575-582, 2006. https://doi.org/10.1016/B0-12-512666-2/00003-1.

Cite this as:

Weisstein, Eric W. "Two-Body Problem." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/Two-BodyProblem.html

Subject classifications